A chip-scale ion-trap mass spectrometer driven by a monolithic photodiode array and a method of fabricating the same. A high-voltage photovoltaic source is located in proximity to the ion-trap mass spectrometer structure. The high-voltage photovoltaic source includes monolithically fabricated and serially connected photodiodes. An external light source illuminates the photodiodes to generate a high voltage across the photodiode array. An RF voltage modulation is attained by modulating the light source at a desired RF frequency. The high-voltage photodiode array may be monolithically fabricated in association with the ion-trap mass spectrometer. The photodiode array requires a small area compared to the ion-trap mass spectrometer size as the spectrometer typically possess a very small capacitance and a low power consumption.
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21. An ion trap mass spectrometer system, comprising:
a ion trap array that provides mass spectroscopy at a operating pressure higher than conventional ITMS, said ion trap array including a cylindrical ring electrode and at least two planar end cap electrodes separated by an insulation layer; and
a photovoltaic source located in proximity to said ion trap array, said photovoltaic source comprising a photodiode array to generate a high radio frequency voltage for trapping ions in a trapping volume defined by said cylindrical ring electrode and said at least two planar end cap electrodes.
1. An ion trap mass spectrometer system, comprising:
a mass spectrometer that provides mass spectroscopy at a high operating pressure, said mass spectrometer including a cylindrical electrode and at least two end cap electrodes separated by an insulation layer; and
a photovoltaic voltage source located in proximity to said mass spectrometer, said photovoltaic voltage source comprising a photodiode array to generate an alternating voltage at a radio frequency for trapping ions in a trapping volume defined by said cylindrical ring electrode and said at least two planar end cap electrodes.
16. A method for configuring an ion trap mass spectrometer system, said method comprising:
configuring a mass spectrometer that provides mass spectroscopy at a high operating pressure;
arranging said mass spectrometer to include a cylindrical electrode and at least two end cap electrodes separated by an insulation layer;
locating a photovoltaic voltage source in proximity to said mass spectrometer; and
modifying said photovoltaic voltage source to include a photodiode array to generate an alternating voltage at a radio frequency for trapping ions in a trapping volume defined by said cylindrical ring electrode and said at least two planar end cap electrodes.
9. An ion trap mass spectrometer system, comprising:
a mass spectrometer that provides mass spectroscopy at a high operating pressure, said mass spectrometer including a cylindrical electrode and at least two end cap electrodes separated by an insulation layer;
a photovoltaic voltage source located in proximity to said mass spectrometer, said photovoltaic voltage source comprising a photodiode array to generate an alternating voltage at a radio frequency for trapping ions in a trapping volume defined by said cylindrical ring electrode and said at least two planar end cap electrodes; and
a light source for illuminating said photodiode array to generate said alternating voltage at radio frequency across said photodiode array.
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This application claims priority to U.S. Provisional Patent Application No. 61/285,540, filed on Dec. 11, 2009 entitled “Ion-Trap Mass Spectrometer Driven by a Monolithic Photodiode Array,” and which is hereby incorporated by reference in its entirety.
Embodiments are generally related to spectrometers. Embodiments are additionally related to ion-trap mass spectrometers. Embodiments are also related to monolithic photodiodes and chip-scale electronic components.
A sensitive and versatile analytical system, capable of identifying both large and small molecules and determining their molecular structure, is required to address the complex mixtures of molecules found in many types of chemical and biological problems. Mass spectrometry is a technique of obtaining information regarding the mass of specimen molecules by ionizing the molecules into charged particles for identifying the species of the molecule. In high performance mass spectrometry, it is desired to obtain the best possible accuracy in determining the composition of the sample or molecule that is being measured.
An ITMS (Ion Trap Mass Spectrometer) is a potentially powerful tool for the analysis of biopolymers. An ITSM utilizes electrostatic fields to trap ions in a small volume. Advantages of an ITSM include its compact size and its ability to trap and accumulate ions to increase the signal-to-noise ratio and sensitivity of a measurement. The performance of the ITSM is generally dependent on radio frequency (RF) voltage and frequency.
Miniature mass spectrometers utilized in non-laboratory and harsh environments are of interest for continuous on-line and other monitoring tasks. For miniaturized ion traps, such as chip-scale ion trap arrays fabricated on a silicon wafer, the required RF frequency may be 100 MHz to 1000 MHz, while the voltage amplitude may be maintained at several hundred volts. The large voltage swing at a high frequency presents a difficulty in coupling and transmitting the RF power to distributed ion traps on the chip due to large parasitic losses. Additionally, the drive frequency of the ion trap must be increased to detect the low mass ions and maintain resolution as the ion trap dimensions are decreased. Therefore, the trapping of ions in a micro scale trap is difficult. Furthermore, it can be nearly impossible to construct large arrays of a small ITMS in a chip-scale size for mass trapping of ions.
Based on the foregoing, it is believed that a need exists for an improved chip-scale ion-trap mass spectrometer. A need also exists for an improved RF source in proximity with the ITMS, which can be a monolithic photodiode array as described in greater detail herein.
The following summary is provided to facilitate an understanding of some of the innovative features unique to the disclosed embodiments and is not intended to be a full description. A full appreciation of the various aspects of the embodiments disclosed herein can be gained by taking the entire specification, claims, drawings, and abstract as a whole.
It is, therefore, one aspect of the disclosed embodiments to provide for a micro-scale mass spectrometer capable of mass spectroscopy at high operating pressures.
It is another aspect of the disclosed embodiments to provide for an improved ITMS.
It is a further aspect of the disclosed embodiments to provide for a novel monolithic photodiode array located in proximity with an ITMS and capable of generating high voltage at radio frequency
It is yet another aspect of the disclosed embodiments to provide a method for monolithically fabricating a photodiode array in association with an ITMS.
The aforementioned aspects and other objectives and advantages can now be achieved as described herein. A micro-scale spectrometer (e.g., ITMS) is disclosed, which is driven by a monolithic photodiode array. A method of fabricating such a spectrometer is also disclosed. In general, a high-voltage photovoltaic source can be located in proximity with the spectrometer structure. The high-voltage photovoltaic source is generally configured to include a large number of monolithically fabricated and serially connected photodiodes. An external light source (e.g., light emitting diode, laser diode, etc) can be utilized to illuminate the photodiodes in order to generate a high voltage across the photodiode array. An RF voltage modulation may be attained by modulating the light source at a desired RF frequency. The high-voltage photodiode array can be monolithically fabricated in association with the spectrometer. The photodiode array requires a small area compared to the ion-trap mass spectrometer size as the spectrometer typically possess a very small capacitance and low power consumption.
The spectrometer may be configured to include a cylindrical ring electrode and two planar end cap electrodes. Ions can be trapped in a trapping volume defined by the cylindrical ring electrode and the end cap electrodes. The spectrometer can be energized by the high-voltage photovoltaic source that provides the RF voltage between the two end cap electrodes and a RF drive voltage between the ring electrode and the end cap electrodes for trapping of the ions.
The fabrication of the spectrometer in association with the photodiode array includes the formation of a p-n junction on a substrate (e.g. SOD utilizing an implant, a diffusion, or an epitaxial approach. The p-n junction may be etched in order to form individual photodiodes. An insulation layer can be formed in order to electrically insulate the sidewalls from the electrical interconnects. The ion traps structures are interconnected in order to form, for example, an ITMS array. Further, the photodiode may be monolithically fabricated and serially connected in order to form the photodiode array. The photodiode array can in turn be fabricated with an individual spectrometer structure. The photodiode array permits, for example, a high voltage swing at 10-1000 MHz and the resulting high output impedance closely matches the ion trap. Such an approach can be utilized to fabricate a miniature or a micro scale spectrometer (e.g., ITMS) structure as an individual and/or an array device, which can be utilized for applications such as, for example, mobile gas detection, chemical and biological analysis, and so forth.
The accompanying figures, in which like reference numerals refer to identical or functionally-similar elements throughout the separate views and which are incorporated in and form a part of the specification, further illustrate the present invention and, together with the detailed description of the invention, serve to explain the principles of the disclosed embodiments.
The particular values and configurations discussed in these non-limiting examples can be varied and are cited merely to illustrate at least one embodiment and are not intended to limit the scope thereof.
The mass spectrometer 100 generally includes a cylindrical ring electrode 130 and two planar end cap electrodes 120 and 125. The ions can be trapped in a trapping volume 115 defined by the cylindrical ring electrode 130 and the end cap electrodes 120 and 125. The ring electrode 130 and the endplate electrodes 120 and 125 on either sides of the ring electrode 130 can be bonded in such as way that these electrodes 120, 125 and 130 can be electrically insulated from each other. The mass spectrometer 100 can be energized by a photovoltaic source 180 that provides an RF voltage between the two end cap electrodes 120 and 125 and a RF drive voltage between the ring electrode 130 and the end cap electrodes 120 and 125 for trapping of the ions. Such an on-site RF generation eliminates transmission loss.
The photodiode array 150 comprises a large number of monolithically fabricated and serially connected photodiodes such as a photodiode 155. In general, the photodiode array is a linear array of discrete photodiodes capable of converting light into either current or voltage, depending upon the mode of operation. When a photon of sufficient energy strikes the photodiode 150, it excites an electron, thereby creating a mobile electron and a positively charged electron hole. The photodiode 155 produces an electrical signal in a known manner as a result of light being incident thereon which is produced by, for example, a light source 110. The electrical signal generated by the photodiode array 150 can be supplied to the mass spectrometer 100.
The high voltage can be transmitted via the electrodes 120, 125 and 130 to the ion trapping volume 115. Apertures 160 and 165 can be provided in association with the electrodes 120 and 125 for injection of a neutral or ionized sample gas and ejection of the ions from the ion trap 115. The output impedance of the photodiode array 150 may closely match the ion trap. A DC bypass inductor 190 may be monolithically implemented to prevent DC bias on the trap. Varying the RF frequency or voltage can selectively destabilize ions and cause ejection through the aperture 160. The ejected ions can then be collected and measured by a low-current amplifier (such as an electron multiplier, not shown) and suitable signal processing methods for further applications. Since, the mass spectrometer 100 typically has small capacitance and power consumption, the photodiode array 150 need a small area compared to the ion trap mass spectrometer size.
A p-n junction, for example, can be initially formed on the SOI (Silicon on Insulator) substrate 330 utilizing an implant or epitaxial technique, as depicted in the process step 303 of
The p-n junction layer 310 and 320 can be etched, as illustrated in
Next, as indicated by the processing step 305 depicted in
The photodiode array 150 can be monolithically fabricated to the individual ion trap mass spectrometer 100 in order to form the ion trap mass spectrometer array 700, as depicted in
The ion traps structures can be interconnected to form the ion trap mass spectrometer array structure 700, as illustrated at block 840. Thereafter, the individual photodiode 150 can be connected to form the photodiode array 150, as depicted at block 850. The photodiode array 150 can be monolithically fabricated in association with each ion trap mass spectrometer 100, as indicated at block 860. Next, as illustrated at block 870, the photodiode array 150 can be illuminated via the external light source 110 in order to generate on site high RF frequency 105. The ions can be therefore trapped within the ion trap 115 utilizing the high RF frequency, as depicted at block 880.
The photodiode array 150 enables high voltage modulation at 10-1000 MHz and the high output impedance closely matches the ion trap. Such an approach 800 can be utilized to fabricate a miniature or a micro scale ITMS structure as an individual and/or an array device. The mass spectrometer array 700 can be utilized for the chemical analysis of known and unknown compounds due to its ability to effectively analyze large as well as small molecules. The mass spectrometer array 700 can further be utilized for applications such as portable or mobile gas detection, chemical and biological analysis, environmental monitoring, protein synthesis and DNA sequencing and so forth.
Based on the foregoing, it can be appreciated that in an embodiment, an ion trap mass spectrometer system can include a mass spectrometer that provides mass spectroscopy at a high operating pressure. The mass spectrometer can be configured to include a cylindrical electrode and two or more end cap electrodes separated by an insulation layer. In such an embodiment, a photovoltaic voltage source can be located in proximity to the mass spectrometer, the photovoltaic voltage source comprising a photodiode array to generate an alternating voltage at a radio frequency for trapping ions in a trapping volume defined by the cylindrical ring electrode and the planar end cap electrodes.
In another embodiment of such a system a light source can be provided for illuminating the photodiode array to generate the alternating voltage at radio frequency across the photodiode array. The light source can be modulated at a desired radio frequency to attain a radio frequency voltage modulation. In some embodiments of such a system, the photodiode array can include a plurality of serially connected photodiodes. In other embodiments, the photodiode array can be monolithically fabricated in association with the mass spectrometer. In another embodiment, the mass spectrometer in association the photodiode array can be fabricated to form an array with respect to the mass spectrometer structure. In still a further embodiment of such a system, the mass spectrometer structure can generate an on-site radio frequency to eliminate transmission loss. Additionally, the cylindrical ring electrode and the planar end cap electrodes can be electrically connected via an inductor, such as the by-pass inductor 190 indicated earlier.
It can be further appreciated that an embodiment is disclosed of a method for configuring the disclosed ion trap mass spectrometer system. Such a method can include, for example, configuring a mass spectrometer that provides mass spectroscopy at a high operating pressure, arranging the mass spectrometer to include a cylindrical electrode and two or more end cap electrodes separated by an insulation layer, locating a photovoltaic voltage source in proximity to the mass spectrometer, and modifying the photovoltaic voltage source to include a photodiode array to generate an alternating voltage at a radio frequency for trapping ions in a trapping volume defined by the cylindrical ring electrode and the planar end cap electrodes.
In another embodiment of such a method, operations can be performed including providing a light source for illuminating the photodiode array to generate the alternating voltage at radio frequency across the photodiode array, modulating the light source at a desired radio frequency to attain a radio frequency voltage modulation, and electrically connecting the cylindrical ring electrode and the planar end cap electrodes via an inductor. Other processing steps include, but are not limited to, for example, configuring the photodiode array to include a plurality of serially connected photodiodes.
It will be appreciated that variations of the above-disclosed and other features and functions, or alternatives thereof, may be desirably combined into many other different systems or applications. Also that various presently unforeseen or unanticipated alternatives, modifications, variations or improvements therein may be subsequently made by those skilled in the art which are also intended to be encompassed by the following claims.
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